Zahlavi

Research

Rutherford Backscattering Spectrometry

Rutherford Backscattering spectrometry (RBS) is most commonly used non-destructive nuclear analytical methods. RBS is widely used for study of thin layers and for study of multilayer systems with thickness from nm to µm. RBS is very suitable for elemental depth analysis. From such measurement it is possible to determine, with some limitations, both the atomic mass and concentration of elemental target constituents as a function of depth below the surface.

Measurement with this method may be performed on amorphous as well as crystalline materials. It involves measurement of the numbers and energy distribution of energetic ions (usually MeV light ions such He+) backscattered from atoms within the near-surface region of solid targets. Ions for RBS are usually light ions (H+, He+) with energy units MeV.

Energy of backscattered ions, which we detect, is connected with energy loss in scattering on the elements nucleus and with the energy loss of ions between passing through the sample. The RBS detection limit is between 1011 – 1015 at.cm-2. RBS depth resolution is an average of 5 nm.

Features of RBS:

  • high sensitivity for heavy elements on a light substrates
  • good detection sensitivity for light elements in a heavy matrix only in special cases
  • good depth resolution (average 5 nm)

Parameters of RBS:

  • ions: H+, He+
  • energy of ions: order of MeV
  • detection limit: up to 1mg/g
  • depth range: about micrometer

Theory of RBS

Sample is irradiated with light ions (usually 2-3 MeV (H+or He+)) and the elastically backscattered projectiles at large angles are detected. The mass of the target atoms could be identified from the energy of the backscattered projectile. The backscattered particles are detected by the semiconductor detectors Si(Au), the accessible depth 2-10 mm. The heavy element detection limit in the light matrix is up to 1mg/g. The lower mass causes higher transferred energy. The mass resolution is given by detector energy resolution, the energy and projectile mass. The ussage of heavier ions enables us to reach the mass resolution DM<2.

Elastic Recoil Detection Analysis and Time of Flight ERDA

Elastic Recoil Detection Analysis (ERDA) is a non-destructive nuclear analytical method. ERDA is a technique for depth profiling of light elements in thin layers and in multilayer systems. Measurement with this method may be performed on amorphous as well as crystalline materials. ERDA uses high energy (~1MeV/amu) heavy-ion beams to kinematically recoil and depth profile low atomic number target atoms. The heavy ion projectile only needs to have a greater mass than the target atom. Alpha particles are commonly used to obtain recoil spectrum for hydrogen and its isotopes.

Features of ERDA:

  • good sensitivity for light elements
  • wors mass resolution
  • good depth resolution (average 10 nm)

Parameters of RBS:

  • ions: He+ and heavy ions
  • energy of ions: order of MeV for He+ and order of 10 MeV for heavy ions
  • detection limit: 1mg/g
  • depth range: order 100 nm

Time of flight ERDA

The mass-depth ambiguity can complicate the interpretation of ERDA spectra. This ambiguity results because the energy of the recoiled ions depends on the mass and depth of the target atom in the sample. Here is a benefit of Time of flight - ERDA (TOF-ERDA), the recoil ion energy and mass we can measured independently. TOF-ERDA measured simultaneous the velocity and energy of the recoiled atoms from the target. The velocity of recoil atoms is determined by measuring the time required to pass between two thin foils at TOF1 ad TOF2 with a corresponding TOF distance. As the atoms passes through the foil, secondary electrons are ejected and accelerated into detector to mark a timing event.

Ions for TOF-ERDA ranging from O to Au at tens of MeV.

RBS channeling

RBS-channeling spectrometry - enables us to investigate crystalline materials. RBS channeling is based on channeling of charged particles in monocrystalline grid of sample. Path of ions that browse through crystals is reduced by crystalline grid. Most of incident ions is caught inside the channels from atoms string. These atoms are further dispersed inside channels on great angle. For RBS channeling are typical ion beams with 1-2MeV He+ ions that are suitable for good mass and depth resolution and small radiation damage.

The signal of the impurity and host lattice in RBS spectra is separated by scattering kinematics . The angular yield curve (scan) is obtained by monitoring the yield of the impurity and host lattice along the channeling axis using ion beam impact angle changing. From the angular yield curves of the axial channels in virgin material we obtain the impurity position in the measured cut. In order to determine the lattice position of impurities several relevant crystallographic directions have been selected.

 

PIXE, PIGE and PESA

Particle Induced X-Ray Spectroscopy (PIXE) is a very sensible non-destructive ion beam analytical method for elemental composition study. PIXE is very suitable for a study of area and bulk concentration of elements not for depth analysis. Basees for this method is that the high energetic proton beam excites, due to inner-shell ionization, the emission of characteristic X-rays from the sample atoms. Particle Induced Gamma-ray Spectroscopy (PIGE) is a versatile technique, which complements other ion beam techniques (especially PIXE) for sample analysis. It is the most common application of nuclear analysis. The PIGE method is mostly based on nuclear reactions (p, g), (p,p´g), (p, a g) induced by MeV protons, where prompt nuclear gamma-rays are produced. PIGE is very suitable for light elements analysis.

In the true sense, PIXE is not a nuclear technique, since the ionisation of the atoms by the ion beam and the subsequent emission of characteristic X-rays are purely atomic electromagnetic processes. Great benefit of PIXE is possibility of measurement at atmospheric pressure.

Features of PIXE and PIGE:

  • high sensitivity
  • measurement at atmospheric pressure

Parameters:

  • ions: H+
  • energy of ions: order of MeV
  • detection limit: up to 100 ppm (PIXE), 1000 ppm (PIGE)
  • depth range: order of ten micrometer

 
Ion Micro-beam

Basic idea of this method is focusing of a ion beam on the smallest dimension and scanning on the sample. Ion beam analytical methods are the same as with normal dimensions – classical ion beam methods (RBS, PIXE, PIGE). Ion micro-beam is versatile equipment that allows study of structures with resolution of microns. Compared to electron micro-beam have better detection limits and may study the trace quantity. Moreover one can use micro-beam for other application like proton writing.

Beam characteristic

Objects slits to sample   5m    
Objects slits to collimator   4m    
    Typical current
Objects slits (openning alternativelly)   20x80 µm2   40-50 pA
  30x120 µm2   70-100 pA
  40x160 µm2   100-200 pA
with sputter source   60x240 µm2   50-100 pA
Collimator slits   800x800 µm2    
Energy (standart)   2 MeV    
Other tested   from 0.8 MeV to 2.6 MeV (11.5 MeV for C4+)
Ions (tested)   H+, He+,C4+
Typical brightness (2 MeV protons)
Duoplasmatron   0.4 pA/µm2 mr2 MeV
Cs sputter source   0.1 pA/µm2 mr2 MeV

 
Ion beam implantation

Ion beam implantation is a process when accelerated ions are shooting into the solid. This methods is optimal for change of physical, chemical, electric or optic properties of the solid. Ion beam implantation is capable of preparation of layers with high density and good defined depth profile and for change of crystalline structure of substrate.

Application of ion beam implantation:

  • doping of semiconductors
  • doping of insulators with metal ions
  • creation of nanoparticles
  • change of electric and optic properties of solid

The typically produced ion beams available at Tandetron facility are provided in the table with the appropriate ion beam currents. The additionally requested ions for your experiments must be consulted with the instrument responsible and tested before the experiment will be proposed at Tandetron in the frame of CANAM.

 
Functional prototypes and software

LabView code for automatic control of the four-axis manipulator designed for structural studies using nuclear analytical methods

Authors:

Ing. Jiří Novotný, A. Macková, P. Malinský

Annotation:

In the frame of instrumentation development for nuclear analytical methods was installed the sophisticated four-axis goniometer for sample manipulation. Structural studies using nuclear analytical methods need software which enables the automatized procedures of the movements for the finding of the main crystallographic orientations. The goniometer offers the lateral movements in two axes, measuring of the larger set of samples and the rotation around the horizontal and vertical axis. The movements of all four stepper motors can be used in both relative and absolute mode. To determine the absolute position of all axes are used in rotation position sensors and X and Y are used terminal micro switch. Position of all axes is graphically and numerically watched on a computer monitor. Motor movements can be carried out continuously or the movements are realized precisely to the given value with the precision 0.01°. The predefined geometrical arrangements can be used Zero-pos, TOF, ERDA, LOAD-LOCK, and RBS10 Thru and allow approaching the specific measurement position. In the frame of this code is it possible to use the automatized procedures of the crystalline material scanning with simultaneous measurement of the back-scattered ions (RBS) or X-rays (PIXE). Based on this scanning procedure we can find interactively the main crystallographic axis of the investigated crystalline sample and used it for the further structural study. Simultaneously, these positions are monitored virtual LEDs. The program is unique because the manipulator is designed especially for this purpose.

LabView program for surface resistivity measurements of samples

Authors:

Ing. Jiří Novotný, Ing. Pavel Horák, Václav Kučírek

Annotation:

The program is designed for the measurement of the sample sheet resistivity using the van der Pauw method, i.e. the 4-point resistivity measurement. The arrangement is designed for square samples with dimensions 15x15 and 12x12 mm. The program communicates with the switch, power source and voltmeter Keithley and calculates the surface resistance of the samples (see Appendix). The electric current set in the program is driven to 2 adjacent electrodes and voltage is measured on remaining 2 electrodes. The measurement is repeated with reversed polarity. Subsequently, the switch disconnects current setup and connects new set of contacts. The electrical current is driven in the same way and the voltage is measured. All 4 sides of the sample are being measured this way and 8 values of the resistance are obtained. From these values a value of sheet resistivity is calculated.

Automatic measuring system for simultaneous analysis PIXE, RBS, PIGE and PESA on LabWiew base for XIA digital modules Pixie4 and XMAP

Authors:

Ing. Jiří Novotný, RNDr. Havránek Vladimír CSc.

Annotation:

This Lab Wiew computer code enables both fully manual and automatic control over the IBA (Ion Beam Analysis) measurement (mainly individual or simultaneous measurements by PIXE, RBS, PIGE and PESA methods ) in multipurpose target chamber placed on the Tandetron 4130MC ion beam line +30o at INP ASCR. The cod controls adjustments of the samples into the measuring position by means of 4-axis manipulator. It communicates with XIA (Pixie4 and XMAP) digital modules and   controls acquisition and visualization of spectra from up to 8 spectroscopic lines . The cod registers ion beam intensity and ion fluences during and after the measurement by means of inner and external beam monitor and   check the sample position and condition after the measurement using digital camera. Finally, it controls the archiving of measured spectra and measurement condition in format suitable for subsequent analysis. This measuring system considerably improves and speed up the analysis , storage and arranging of measured data, and simplifies further spectral data evaluation. The cod is suitable, both for the individual sample measurement or for the measurement of large series of samples.

The system of corrective magnets

Authors:

V. Kučírek, J. Novotný, V. Semián

Annotation:

It is a system of corrective magnets with appropriate power source for correcting of the ion beam axis to achieve the optimal beam trajectory for passing through the collimator which axis does not correspond exactly with the geometry of the beam line. By this way it may be optimalized the beam direction into 4 different ion beam lines. Central control is possible from the PC via RS232 serial port.

LabView program for implantation to 12 samples and to center the beam during implantation

Authors:

Ing. Jiří Novotný, RNDr. Vladimír Havránek, CSc.

Annotation:

This is software dedicated for an automatic ion implantation of set of samples as an extension for an implantation chamber commercially manufactured by High Voltage Ltd. In the chamber, there is a manually rotated carousel for 12 samples and four Faraday cups are used for ion current measurements. Automatic sample implantation is realized using a stepping motor connected to the chamber; to indicate the sample in the implant position micro switches are used. The programme (written in LabView, Austin, USA) needs input data: the terminal voltage of the accelerator, ion charge and the required fluence ions/cm2, which is entered into a table for each sample. The programme calculates the implantation parameters for set input data and evaluates its viability as a electrostatic steering of ion beam in X and Y,  the number of pulses of the integrator. Further, the program operates the Faraday Cup located in the beamline for the beginning and the end of the implantation. During implantation, the following values are displayed: ion energy, the estimated time of implantation, current (nA/cm2), real counts,  implanted fluence (ions/cm2), the time until the end of implantation, the current position of the carousel and the LED display of the sample position. For the event of a shutdown status of the implantation is every minute written into a file. At the end of the implantation is the implantation protocol written into the same file.

For the positioning of the beam over the sample, the programme graphically shows the calculated location of four Faraday cups and determines the geometric centre, to which the sample for the implantation is placed.

This software improves significantly the implantation procedure; saving the processing time of the accelerator during the implantation. It does not require the presence of the operator, thus lowering the costs of the sample implantation.

LabView program for Profile Beam Monitor

Authors:

Ing. Jiří Novotný, RNDr. Vladimír Havránek, CSc.

Annotation:

The functional sample program is expanding the commercial Beam Profile Monitor from NEC Ltd. Originally, the monitor had to be connected to an oscilloscope and it was quite complicated to measure the ion beam profile. The program (written in Labview, Austin, USA) replaced the oscilloscope and the measurement became simpler and clearer. The programme displays peaks in planes X and Y, color-coded quantity of cutting axes X and Y, and the integral spectrum in X and Y.

Since it is not necessary to connect to the oscilloscope, the information about the shape and location of the ion beam is quickly graphically indicated, saving the operator time and the machine time of the accelerators.

Software for the positioning during the irradiation on the external beam

Authors:

Ing. Jan Vitner, M. Davidkova

Annotation:

SW is used for precise positioning of samples exposed to the ion beam radiation in the ambient atmpsphere. There is a positioning device driven by two electromotors, which are controlled by the developed SW. SW allows us to control the positioning device in precision about 0,001 mm in two axis, thus the areal scanning is available. Thus we are able to irradiate the samples, which can not be placed in vacuum conditions (e.g. living cells), with the defined mathematical procedure to cover the requested irradiation area homogeneously by ion beam with maximum beam spot 1 mm2 . We can choose the size of the area exposed to the radiation, to choose the quantity of the radiation (ion fluence) and to achieve uniform radiation of the sample with very low fluencies 104 iontů/cm-2.

stolek stolekf

The gate of the ion beam

Authors:

Václav Kučírek, Vladimír Havránek RNDr., CSc., Vladimír Semián, Pavel Plocek

Annotation:

It is a source of pulses plus and minus one hundred volts with a very short rising and falling edge (less than 0.2 microseconds). Normally, the output is exactly at zero. Pulses can be of any length. The pulses are fed to the deflection plates. During the deflection the beam does not pass through the ion line but ends on the screens. Actuating: TTL signal.

gate gate13

Indicator of neutron flux

Authors:

Václav Kučírek, Jiří Vacík Ing., CSc.

Annotation:

It is uni-module unit NIM comprising eight highly stable sources of spectrometric pulses with independently adjustable polarity and independently adjustable amplitude from zero to five volts. The device further includes a spectrometric amplifier and the related upper discriminator. From the output of the discriminator the output pulses are synchronized. To synchronize the output pulses is also possible to use external pulses or internal generator.

Internal television system

Authors:

J. Kučírek, J. Novotný, V. Semián

Annotation:

It is a closed television system for distributing signals from many cameras to two output channels, and also on several monitors. The system can be independently controlled from multiple locations including several lines RS232.

tv tv1

Beam Current Measuring System of the Shadowing Shields

Authors:

Ing. Jan Vitner, Václav Kučírek, Ing. Martin Švider, Pavel Plocek, Vladimír Semián

Annotation:

The system is used for the measuring of an accelerator beam of particles. There are four movable shields placed across the beam line in two rectangle axes in all directions. The beam can be falling to each of them by its small part. Each shield can evoke a current flowing between the shield and the developed measuring device. The device is able to measure the current flowing from each of those shields and the device is able to screen measured data by itself or the data could be send to an computer to be screened by a special program, which is an component of the whole developed system. Thanks to this system, we are able to center the beam. The output information is the value of the current flowing from each shield, which represents the value of the charge fallen to the current shield.

clony Schema